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arXiv 0907.5113astro-ph.SR
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Herbig Ae星V380 Ori的磁性和双星性

Magnetism and binarity of the Herbig Ae star V380 Ori

E. Alecian, G. A. Wade, C. Catala, S. Bagnulo, T. Böhm, J. -C. Bouret, J. -F. Donati, C. P. Folsom, J. Grunhut, J. D. Landstreet

摘要:

在本文中,我们报告的结果,高分辨率圆偏振光谱监测的Herbig Ae星V380猎户座,其中我们发现了一个磁场在2005年。对强度谱的仔细研究揭示了一个冷的光谱伴侣的存在。通过模拟的二进制光谱,我们推断出两颗恒星的有效温度:$10500\pm 500$ K的主要,和$5500\pm500$ K的次要,我们认为,高金属丰度($[M/H] = 0.5$),需要适合线可能意味着,主要是一个化学奇特的明星。我们观察到次级线的径向速度随时间变化,而初级线的径向速度不随时间变化。通过拟合这些变化,我们得到系统的轨道参数。我们发现$104\pm5$的轨道周期为d,质量比($M_{\rm P}/M_{\rm S}$)大于2.9。强度谱被强、宽和可变的发射严重污染。对这些线的简单分析表明,一个圆盘可能围绕着双星,并且在系统的环境中发生了风。最后,我们进行了磁分析,使用最小二乘解卷积(LSD)的配置文件的斯托克斯$V$光谱的两颗星,并采用斜转子模型。从旋转调制的主要的斯托克斯$V$签名,我们推断其旋转周期$P=4.31276\pm0.00042$ d,并发现它主机的极性强度$2.12\pm0.15$ kG的中心偶极磁场,与磁性$β= 66\pm5^{\circ}$,和旋转轴倾角$i=32\pm5^{\circ}$。然而,在次级中没有检测到磁场,如果它拥有偶极磁场,它的强度必须低于约500 G,才能与我们的观测结果一致。

英文摘要:

In this paper we report the results of high-resolution circular spectropolarimetric monitoring of the Herbig Ae star V380 Ori, in which we discovered a magnetic field in 2005. A careful study of the intensity spectrum reveals the presence of a cool spectroscopic companion. By modelling the binary spectrum we infer the effective temperature of both stars: $10500\pm 500$ K for the primary, and $5500\pm500$ K for the secondary, and we argue that the high metallicity ($[M/H] = 0.5$), required to fit the lines may imply that the primary is a chemically peculiar star. We observe that the radial velocity of the secondary's lines varies with time, while that of the the primary does not. By fitting these variations we derive the orbital parameters of the system. We find an orbital period of $104\pm5$ d, and a mass ratio ($M_{\rm P}/M_{\rm S}$) larger than 2.9. The intensity spectrum is heavily contaminated with strong, broad and variable emission. A simple analysis of these lines reveals that a disk might surround the binary, and that a wind occurs in the environment of the system. Finally, we performed a magnetic analysis using the Least-Squares Deconvolved (LSD) profiles of the Stokes $V$ spectra of both stars, and adopting the oblique rotator model. From rotational modulation of the primary's Stokes $V$ signatures, we infer its rotation period $P=4.31276\pm0.00042$ d, and find that it hosts a centred dipole magnetic field of polar strength $2.12\pm0.15$ kG, with a magnetic obliquity $β= 66\pm5^{\circ}$, and a rotation axis inclination $i=32\pm5^{\circ}$. However, no magnetic field is detected in the secondary, and if it hosts a dipolar magnetic field, its strength must be below about 500 G, to be consistent with our observations.

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